Paper 1 Thermal Physics Route Answers
| Q | Ans | Brief reason |
|---|
| 1 | B | Thermal equilibrium means no net heat flow and equal temperature. |
| 2 | C | 27+273.15≈300 K. |
| 3 | B | Gas equations require thermodynamic temperature. |
| 4 | B | E=mcΔT. |
| 5 | B | Latent heat changes state without temperature change. |
| 6 | A | Internal energy is microscopic kinetic plus potential energy. |
| 7 | A | Ideal gas equation. |
| 8 | B | First law links ΔU, heating and work. |
| 9 | B | Potential part of internal energy changes during phase change. |
| 10 | B | At fixed V, p∝T in kelvin. |
| 11 | B | ⟨Ek⟩=3kT/2. |
| 12 | B | Heat loss means input energy overestimates useful energy, so calculated c is too large. |
| 13 | B | Adiabatic expansion does work using internal energy. |
| 14 | C | Internal energy depends on state; heat/work are transfers. |
| 15 | B | Wall collisions produce pressure. |
| 16 | B | Thermal equilibrium requires equal temperature and no net thermal energy transfer. |
| 17 | A | The internal energy of a fixed amount of ideal gas is a function of thermodynamic temperature only. |
| 18 | A | Charles law in kelvin. |
| 19 | A | Heat is energy in transit due to temperature difference. |
| 20 | B | Constant-volume gas pressure extrapolates to zero. |